Measurements of the branching fraction ratio ${\cal{B}(\phi \to \mu^+ \mu^-)/\cal{B}(\phi\to e^+e^-)}$ with ${D_{s}^{+} \to \pi^{+} \phi}$ and ${D^{+} \to \pi^{+} \phi}$ decays, denoted $R^{s}_{\phi \pi}$ and $R^{d}_{\phi \pi}$, are presented. The analysis is performed using a dataset corresponding to an integrated luminosity of 5.4$ \rm{fb}^{-1}$ of $pp$ collision data collected with the LHCb experiment. The branching fractions are normalised with respect to the ${B^{+} \to K^{+} J/\psi(\to e^+e^-)}$ and ${B^{+} \to K^{+} J/\psi(\to \mu^+\mu^-)}$ decay modes. The combination of the results yields $$ R_{\phi \pi} = 1.022 \pm 0.012 ({\rm stat}) \pm 0.048 ({\rm syst}). $$ The result is compatible with previous measurements of the $\phi \to \ell^{+}\ell^{-}$ branching fractions and predictions based on the Standard Model.
Distribution of the invariant mass $ m_{\phi}{(\pi ^+ \ell^+ \ell^- )}$ overlaid with the result of the fit for candidates with (left) muon and (right) electron pairs in the final states. The dotted and dot-dashed lines describe the signal contributions, while the solid areas represent the background components. |
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Left: distribution of the $\pi ^+ \ell^{+}\ell^{-}$ invariant mass of candidates obtained from selecting final states with electrons of same charge (blue) or that fail the BDT requirement (orange). Fit results using a third-order polynomial are overlaid. The overall normalisation is chosen such that the two curves have the same area. Right: distribution of the invariant mass of $\pi^{+}\ell^{-}\ell^{+}$ candidates, after interpreting the leptons as pions, for candidates failing the electron PID criteria. The reversed PID sample contains predominantly $ D^{+}_{(s)}\rightarrow \pi ^+ \pi ^- \pi ^+ $ events and a fraction of combinatorial events. |
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Invariant mass distributions of the selected candidates for the (left) $ { B ^+ \rightarrow K^{+} { J \mskip -3mu/\mskip -2mu\psi } (\rightarrow e ^+ e ^- )}$ and (right) $ { B ^+ \rightarrow K^{+} { J \mskip -3mu/\mskip -2mu\psi } (\rightarrow \mu ^+\mu ^- )}$ modes, overlaid with the result of the fit. The dotted lines describe the signal contribution and the solid areas represent each of the background components described in the text. |
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Distributions of (top) $m(e^{+}e^{-})$ and (bottom) $m(\mu^{+}\mu^{-})$ for candidates selected in the signal region of the (left) $ D ^+$ (right) and $ D ^+_ s $ $\phi$-constrained invariant mass. The dotted lines describe the signal contribution and the solid areas represent each of the background components described in the text. |
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Distribution of the invariant mass computed under the pion mass hypothesis for the dielectron pair using track information only, for candidates passing the electron PID criteria. The fit projection is superimposed, with dashed and dotted-dashed lines describing the signal contributions, while solid light and dark blue areas represent misidentified $ D^{+}_{(s)}\rightarrow \pi ^+ \pi ^- \pi ^+ $ components. In this variable the latter are clearly visible in data passing the electron PID criteria. |
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Measured $ R^{(d,s)}_{\phi \pi}$ as a function of the (top left) angle between the leptons $\alpha(\ell^+, \ell^-)$, and (top right) the maximum $ p_{\mathrm{T}}$ of the leptons. The structure observed at intermediate maximum $ p_{\mathrm{T}}$ is related to the trigger threshold. The errors shown are statistical only. Also shown is the ratio of efficiency-corrected ${ D^{+}_{(s)} \rightarrow \pi ^+ \phi }$ and ${ { B ^+ \rightarrow K^{+} { J \mskip -3mu/\mskip -2mu\psi } (\rightarrow e ^+ e ^- )} }$ yields as a function of the (bottom left) transverse momentum recovered with the bremsstrahlung recovery algorithm and (bottom right) its fraction with respect to the total transverse momentum of the electron. The flatness of these distributions indicates that the bremsstrahlung recovery algorithm is well reproduced in simulation at low $ q^2$ . The normalisation of these distributions is arbitrary and the uncertainties displayed are statistical only. |
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Animated gif made out of all figures. |
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Signal ( $ D^{+}_{(s)} \rightarrow \pi ^+ \phi$ ) and normalisation ( $ { B ^+ \rightarrow K^{+} { J \mskip -3mu/\mskip -2mu\psi } (\rightarrow \ell^{+}\ell^{-})}$ ) mode sideband mass ranges. The variables $ m_{\phi}{(\pi ^+ \ell^+ \ell^- )}$ and $ m_{ { J \mskip -3mu/\mskip -2mu\psi } }{( K ^+ \ell^+ \ell^- )}$ are used for signal and normalisation decays, respectively. |
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Yields of the signal and normalisation decay modes obtained from the fits to the data. The quoted uncertainty accounts for both statistical and systematic effects. |
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Relative systematic uncertainties in percent affecting the measurements $ R^{d}_{\phi \pi}$ and $ R^{s}_{\phi \pi}$ . |
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Supplementary material full pdf |
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This ZIP file contains supplemetary material for the publication LHCb-PAPER-2023-038. The files are: supplementary.pdf : An overview of the extra figures supplementary.tex : The corresponding TeX source code *.pdf, *.png, *.eps : The figures in various formats |
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Created on 11 May 2024.